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Many of the numerical peculiarities
can be traced back to the fact that
there is no ``good'' discrete Wigner transform as explained in
Section 8.2. Some are minor technical issues,
which can be solved
by increased implementation efforts. However, often
simulations still
use the simple ``standard discretization''
(i.e., first order upwinding
with Frensley's completeness condition for the mesh) and
hazard the consequences.
A good reference where discretizations of the Wigner
function method are compared is
Biegel's PhD thesis [Bie97].
In contrast for the QTBM the choice of discretization
was a non-issue.
Previous: 10.2.4 Effective Mass Model
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R. Kosik: Numerical Challenges on the Road to NanoTCAD